The \(\log {S}\)  factor in the the scrambling time in SYK
has a simple intuitive bulk meaning as the time it takes for a single fermion to fall from the boundary, where the holographic degrees of freedom are located, to the stretched horizon [1]}. But in static patch holography the holographic degrees of freedom  are already located at the stretched horizon.
Therfore there is no \(\log {S}\)  factor in the scrambling time. The scrambling time for an initially simple operator is of the same order as the decay time of the quasinormal modes. In Rindler units that means a time of order unity,
\(\omega _* &\sim & 1, \cr t_* &\sim & \beta = R.\) 
